Author: Uvarov, V.L.
Paper Title Page
MOPS040 Intra-Bunch Energy Spread of Electrons in Powerful RF Linacs for Nuclear Physics Research* 691
 
  • V.V. Mytrochenko, M.I. Ayzatskiy, V.A. Kushnir, A. Opanasenko, S.A. Perezhogin, V.L. Uvarov
    NSC/KIPT, Kharkov, Ukraine
 
  Funding: Ukrainian State program of fundamental and applied studies on the use of nuclear materials, nuclear and radiation technologies in the fields of economics (YaMRT project No. 826/35)
There are some par­ti­cles in RF elec­tron linacs with en­er­gy that may be sig­nif­i­cant­ly dif­fer­ent from that of par­ti­cles with­in a core of the bunch. Loss of these par­ti­cles at av­er­age beam power of tens of kilo­watts can cause ra­di­a­tion and ther­mal prob­lems. Fil­tra­tion of such par­ti­cles dur­ing the ini­tial stage of ac­cel­er­a­tion, at en­er­gies below the thresh­old of pho­tonu­cle­ar re­ac­tions, is im­por­tant. The paper an­a­lyzes sev­er­al ways to per­form such type of fil­tra­tion in the in­jec­tor part of a pow­er­ful elec­tron linac using a RF chop­per or mag­net­ic sys­tems.
 
 
THPS083 Two-channel Mode of Mo-99 Production at an Electron Accelerator 3627
 
  • V.L. Uvarov, A.N. Dovbnya, V.V. Mytrochenko, V.I. Nikiforov, S.A. Perezhogin, V.A. Shevchenko, B.I. Shramenko, A.Eh. Tenishev, A.V. Torgovkin
    NSC/KIPT, Kharkov, Ukraine
 
  High-en­er­gy bremsstrahlung is the main source of iso­topic tar­get ac­ti­va­tion at an elec­tron ac­cel­er­a­tor. The pho­toneu­trons con­cur­rent­ly gen­er­at­ed are gen­er­al­ly con­sid­ered as a back­ground ra­di­a­tion. At the same time, the nat­u­ral ma­te­ri­als en­ter­ing into pho­tonu­cle­ar tar­gets some­times com­prise a mix­ture of sta­ble iso­topes, the atom­ic-num­ber dif­fer­ence of which equals 2. Thus, if the de­sired iso­tope has an in­ter­me­di­ate mass, then at cer­tain con­di­tions, it can be pro­duced on two tar­get nu­clei at once, via (γ,n) and (n,γ) chan­nels. As an ex­am­ple, we in­ves­ti­gate the pos­si­bil­i­ty of in­creas­ing the yield of 99Mo by means of its si­mul­ta­ne­ous pro­duc­tion from 100Mo(γ,n)99Mo and 98Mo(n,γ)99Mo re­ac­tions. The method and the de­vice have been de­vel­oped to pro­vide mea­sure­ments of the 99Mo yield from the nat­u­ral molyb­de­num tar­get as it is placed in­side the neu­tron mod­er­a­tor and with­out the lat­ter. Ex­per­i­ments were per­formed at the NSC KIPT ac­cel­er­a­tor LU-40m at elec­tron en­er­gies rang­ing from 30 to 60 MeV. It is demon­strat­ed that the use of the mod­er­a­tor gives near­ly a 30% in­crease in the 99Mo yield. The ex­per­i­men­tal re­sults are in good agree­ment with the com­put­er sim­u­la­tion data.  
 
THPS084 Modification of the PENELOPE Transport System for HS Simulation of Isotope Production Mode 3630
 
  • V.L. Uvarov, V.I. Nikiforov
    NSC/KIPT, Kharkov, Ukraine
 
  A method has been de­vel­oped for high-speed com­put­ing the pho­tonu­cle­ar iso­tope yield along with the ab­sorbed ra­di­a­tion power in exit de­vices of elec­tron ac­cel­er­a­tor. The tech­nique in­volves a step-by-step cal­cu­la­tion of iso­tope mi­croyield along the pho­ton tra­jec­to­ries. The ap­proach has been re­al­ized in the com­put­er pro­grams based on the PENE­LOPE sys­tem of -2001, -2006 and -2008 ver­sions. For their bench­mark­ing, use has been made of the ex­per­i­men­tal data on ac­tiv­i­ty dis­tri­bu­tions of the 67Cu pro­duced from 68Zn(γ,p)67Cu re­ac­tion in thick zinc tar­gets. The re­sults of sim­u­la­tion using the PENE­LOPE-2006 and -2008 codes are in ex­cel­lent agree­ment with all ex­per­i­men­tal data. At the same time, the PENE­LOPE-2001 com­pu­ta­tions give good agree­ment with the ex­per­i­men­tal re­sults for tar­get ac­ti­va­tion by the elec­tron beam, but sys­tem­at­i­cal­ly un­der­es­ti­mate (~15%) in case of the tar­get ex­posed to bremsstrahlung. The pro­posed tech­nique pro­vides a ~ 104 times high­er com­pu­ta­tion speed as com­pared with the di­rect Monte Carlo sim­u­la­tion of pho­tonu­cle­ar events and that speed is in­de­pen­dent of the re­ac­tion cross sec­tion.